The sign of longitudinal magnetoconductivity in Weyl semimetals due to chiral anomaly has been a subject of intense research [1]}, [2]}, [3]}, [4]}, [5]}, [6]}, [7]}, [8]}, [9]}, [10]}, [11]}, [12]}, [13]}, [14]}. Almost unanimously, the sign of longitudinal magnetoconductivity has been agreed upon to be positive, at least in the limit of weak magnetic fields. However, various factors, such as tilting of the Weyl cones, strain and inhomogeneties in the material, qualitatively affect the LMC in Weyl semimetals. The interplay between various parameters, such as intervalley scattering, tilt, strain induced chiral gauge field, and the external magnetic field, leads to many striking features in both the longitudinal magnetoconductance and the planar Hall conductance of Weyl semimetals, which has been the focus of this work.
